HEAT AND MASS TRANSFER: FUNDAMENTALS & APPLICATIONS 6th Edition in SI Units Yunus A. Çengel, Afshin J. Ghajar Lecture PPT Lecture slides by Mehmet Kanoglu Copyright © McGraw-Hill Education. Permission required for reproduction or display. Chapter Number 1 INTRODUCTION AND BASIC CONCEPTS McGraw-Hill | 2 Objectives • Understand how thermodynamics and heat transfer are related to each other • Distinguish thermal energy from other forms of energy, and heat transfer from other forms of energy transfer • Perform general energy balances as well as surface energy balances • Understand the basic mechanisms of heat transfer, which are conduction, convection, and radiation, and Fourier's law of heat conduction, Newton's law of cooling, and the Stefan– Boltzmann law of radiation • Identify the mechanisms of heat transfer that occur simultaneously in practice • Develop an awareness of the cost associated with heat losses • Solve various heat transfer problems encountered in practice McGraw-Hill | 3 1-1 THERMODYNAMICS AND HEAT TRANSFER Heat: The form of energy that can be transferred from one system to another as a result of temperature difference. Thermodynamics is concerned with the amount of heat transfer as a system undergoes a process from one equilibrium state to another. Heat Transfer deals with the determination of the rates of such energy transfers as well as variation of temperature. The transfer of energy as heat is always from the highertemperature medium to the lower-temperature one. Heat transfer stops when the two mediums reach the same temperature. Heat can be transferred in three different modes: conduction, convection, radiation McGraw-Hill | 4 McGraw-Hill | 5 Application Areas of Heat Transfer McGraw-Hill | 6 Historical Background Kinetic theory: Treats molecules as tiny balls that are in motion and thus possess kinetic energy. Heat: The energy associated with the random motion of atoms and molecules. Caloric theory: Heat is a fluidlike substance called the caloric that is a massless, colorless, odorless, and tasteless substance that can be poured from one body into another It was only in the middle of the nineteenth century that we had a true physical understanding of the nature of heat. Careful experiments of the Englishman James P. Joule published in 1843 convinced the skeptics that heat was not a substance after all, and thus put the caloric theory to rest. McGraw-Hill | 7 1-2 ENGINEERING HEAT TRANSFER Heat transfer equipment such as heat exchangers, boilers, condensers, radiators, heaters, furnaces, refrigerators, and solar collectors are designed primarily on the basis of heat transfer analysis. The heat transfer problems encountered in practice can be considered in two groups: (1) rating and (2) sizing problems. The rating problems deal with the determination of the heat transfer rate for an existing system at a specified temperature difference. The sizing problems deal with the determination of the size of a system in order to transfer heat at a specified rate for a specified temperature difference. An engineering device or process can be studied either experimentally (testing and taking measurements) or analytically (by analysis or calculations). The experimental approach has the advantage that we deal with the actual physical system, and the desired quantity is determined by measurement, within the limits of experimental error. However, this approach is expensive, timeconsuming, and often impractical. The analytical approach (including the numerical approach) has the advantage that it is fast and inexpensive, but the results obtained are subject to the accuracy of the assumptions, approximations, and idealizations made in the analysis. McGraw-Hill | 8 Modeling in Engineering McGraw-Hill | 9 1-3 HEAT AND OTHER FORMS OF ENERGY • Energy can exist in numerous forms such as: ✓ thermal ✓ mechanical ✓ kinetic ✓ potential ✓ electrical ✓ magnetic ✓ chemical ✓ nuclear • Their sum constitutes the total energy E (or e on a unit mass basis) of a system. • The sum of all microscopic forms of energy is called the internal energy of a system. McGraw-Hill | 10 • Internal energy: May be viewed as the sum of the kinetic and potential energies of the molecules. • Sensible heat: The kinetic energy of the molecules. • Latent heat: The internal energy associated with the phase of a system. • Chemical (bond) energy: The internal energy associated with the atomic bonds in a molecule. • Nuclear energy: The internal energy associated with the bonds within the nucleus of the atom itself. McGraw-Hill | 11 Internal Energy and Enthalpy • In the analysis of systems that involve fluid flow, we frequently encounter the combination of properties u and Pv. • The combination is defined as enthalpy (h = u + Pv). • The term Pv represents the flow energy of the fluid (also called the flow work). McGraw-Hill | 12 Specific Heats of Gases, Liquids, and Solids • Specific heat: The energy required to raise the temperature of a unit mass of a substance by one degree. • Two kinds of specific heats: ✓ specific heat at constant volume cv ✓ specific heat at constant pressure cp • The specific heats of a substance, in general, depend on two independent properties such as temperature and pressure. • At low pressures all real gases approach ideal gas behavior, and therefore their specific heats depend on temperature only. McGraw-Hill | 13 • Incompressible substance: A substance whose specific volume (or density) does not change with temperature or pressure. • The constant-volume and constantpressure specific heats are identical for incompressible substances. • The specific heats of incompressible substances depend on temperature only. McGraw-Hill | 14 Energy Transfer Energy can be transferred to or from a given mass by two mechanisms: when is constant: heat transfer and work. Heat transfer rate: The amount of heat transferred per unit time. Heat flux: The rate of heat transfer per unit area normal to the direction of heat transfer. Power: The work done per unit time. McGraw-Hill | 15 1-4 THE FIRST LAW OF THERMODYNAMICS The first law of thermodynamics (conservation of energy principle) states that energy can neither be created nor destroyed during a process; it can only change forms. The net change (increase or decrease) in the total energy of the system during a process is equal to the difference between the total energy entering and the total energy leaving the system during that process. The energy balance for any system undergoing any process in the rate form McGraw-Hill | 16 In heat transfer problems it is convenient to write a heat balance and to treat the conversion of nuclear, chemical, mechanical, and electrical energies into thermal energy as heat generation. McGraw-Hill | 17 Energy Balance for Closed Systems (Fixed Mass) A closed system consists of a fixed mass. The total energy E for most systems encountered in practice consists of the internal energy U. This is especially the case for stationary systems since they don’t involve any changes in their velocity or elevation during a process. McGraw-Hill | 18 Energy Balance for Steady-Flow Systems A large number of engineering devices such as water heaters and car radiators involve mass flow in and out of a system, and are modeled as control volumes. Most control volumes are analyzed under steady operating conditions. The term steady means no change with time at a specified location. Mass flow rate: The amount of mass flowing through a cross section of a flow device per unit time. Volume flow rate: The volume of a fluid flowing through a pipe or duct per unit time. McGraw-Hill | 19 Surface Energy Balance A surface contains no volume or mass, and thus no energy. Thereore, a surface can be viewed as a fictitious system whose energy content remains constant during a process. This relation is valid for both steady and transient conditions, and the surface energy balance does not involve heat generation since a surface does not have a volume. McGraw-Hill | 20 1-5 HEAT TRANSFER MECHANISMS • • • • • • Heat as the form of energy that can be transferred from one system to another as a result of temperature difference. A thermodynamic analysis is concerned with the amount of heat transfer as a system undergoes a process from one equilibrium state to another. The science that deals with the determination of the rates of such energy transfers is the heat transfer. The transfer of energy as heat is always from the higher-temperature medium to the lower-temperature one, and heat transfer stops when the two mediums reach the same temperature. Heat can be transferred in three basic modes: ✓ conduction ✓ convection ✓ radiation All modes of heat transfer require the existence of a temperature difference. McGraw-Hill | 21 1-6 CONDUCTION Conduction: The transfer of energy from the more energetic particles of a substance to the adjacent less energetic ones as a result of interactions between the particles. In gases and liquids, conduction is due to the collisions and diffusion of the molecules during their random motion. In solids, it is due to the combination of vibrations of the molecules in a lattice and the energy transport by free electrons. The rate of heat conduction through a plane layer is proportional to the temperature difference across the layer and the heat transfer area, but is inversely proportional to the thickness of the layer. McGraw-Hill | 22 When x → 0 Fourier’s law of heat conduction Thermal conductivity, k: A measure of the ability of a material to conduct heat. Temperature gradient dT/dx: The slope of the temperature curve on a T-x diagram. Heat is conducted in the direction of decreasing temperature, and the temperature gradient becomes negative when temperature decreases with increasing x. The negative sign in the equation ensures that heat transfer in the positive x direction is a positive quantity. McGraw-Hill | 23 McGraw-Hill | 24 Thermal Conductivity Thermal conductivity: The rate of heat transfer through a unit thickness of the material per unit area per unit temperature difference. The thermal conductivity of a material is a measure of the ability of the material to conduct heat. A high value for thermal conductivity indicates that the material is a good heat conductor, and a low value indicates that the material is a poor heat conductor or insulator. McGraw-Hill | 25 McGraw-Hill | 26 The range of thermal conductivity of various materials at room temperature. McGraw-Hill | 27 The thermal conductivities of gases such as air vary by a factor of 104 from those of pure metals such as copper. Pure crystals and metals have the highest thermal conductivities, and gases and insulating materials the lowest. McGraw-Hill | 28 The variation of the thermal conductivity of various solids, liquids, and gases with temperature. McGraw-Hill | 29 Thermal Diffusivity cp Specific heat, J/kg·°C: Heat capacity per unit mass cp Heat capacity, J/m3·°C: Heat capacity per unit volume Thermal diffusivity, m2/s: Represents how fast heat diffuses through a material A material that has a high thermal conductivity or a low heat capacity will obviously have a large thermal diffusivity. The larger the thermal diffusivity, the faster the propagation of heat into the medium. A small value of thermal diffusivity means that heat is mostly absorbed by the material and a small amount of heat is conducted further. McGraw-Hill | 30 1-7 CONVECTION Convection: The mode of energy transfer between a solid surface and the adjacent liquid or gas that is in motion, and it involves the combined effects of conduction and fluid motion. The faster the fluid motion, the greater the convection heat transfer. In the absence of any bulk fluid motion, heat transfer between a solid surface and the adjacent fluid is by pure conduction. McGraw-Hill | 31 Forced convection: If the fluid is forced to flow over the surface by external means such as a fan, pump, or the wind. Natural (or free) convection: If the fluid motion is caused by buoyancy forces that are induced by density differences due to the variation of temperature in the fluid. Heat transfer processes that involve change of phase of a fluid are also considered to be convection because of the fluid motion induced during the process, such as the rise of the vapor bubbles during boiling or the fall of the liquid droplets during condensation. McGraw-Hill | 32 Newton’s law of cooling h As Ts T convection heat transfer coefficient, W/m2 · °C the surface area through which convection heat transfer takes place the surface temperature the temperature of the fluid sufficiently far from the surface. The convection heat transfer coefficient h is not a property of the fluid. It is an experimentally determined parameter whose value depends on all the variables influencing convection such as - the surface geometry - the nature of fluid motion - the properties of the fluid - the bulk fluid velocity McGraw-Hill | 33 1-8 RADIATION • Radiation: The energy emitted by matter in the form of electromagnetic waves (or photons) as a result of the changes in the electronic configurations of the atoms or molecules. • Unlike conduction and convection, the transfer of heat by radiation does not require the presence of an intervening medium. • In fact, heat transfer by radiation is fastest (at the speed of light) and it suffers no attenuation in a vacuum. This is how the energy of the sun reaches the earth. • In heat transfer studies we are interested in thermal radiation, which is the form of radiation emitted by bodies because of their temperature. • All bodies at a temperature above absolute zero emit thermal radiation. • Radiation is a volumetric phenomenon, and all solids, liquids, and gases emit, absorb, or transmit radiation to varying degrees. • However, radiation is usually considered to be a surface phenomenon for solids. McGraw-Hill | 34 Stefan–Boltzmann law = 5.670 10−8 W/m2 · K4 Stefan–Boltzmann constant Blackbody: The idealized surface that emits radiation at the maximum rate. Radiation emitted by real surfaces Emissivity : A measure of how closely a surface approximates a blackbody for which = 1 of the surface. 0 1. McGraw-Hill | 35 Absorptivity : The fraction of the radiation energy incident on a surface that is absorbed by the surface. 0 1 A blackbody absorbs the entire radiation incident on it ( = 1). Kirchhoff’s law: The emissivity and the absorptivity of a surface at a given temperature and wavelength are equal. McGraw-Hill | 36 Net radiation heat transfer: The difference between the rates of radiation emitted by the surface and the radiation absorbed. The determination of the net rate of heat transfer by radiation between two surfaces is a complicated matter since it depends on • the properties of the surfaces • their orientation relative to each other • the interaction of the medium between the surfaces with radiation When a surface is completely enclosed by a much larger (or black) surface at temperature Tsurr separated by a gas (such as air) that does not intervene with radiation, the net rate of radiation heat transfer between these two surfaces is given by Radiation is usually significant relative to conduction or natural convection, but negligible relative to forced convection. McGraw-Hill | 37 When radiation and convection occur simultaneously between a surface and a gas: Combined heat transfer coefficient hcombined Includes the effects of both convection and radiation McGraw-Hill | 38 1-9 SIMULTANEOUS HEAT TRANSFER MECHANISMS Heat transfer is only by conduction in opaque solids, but by conduction and radiation in semitransparent solids. A solid may involve conduction and radiation but not convection. A solid may involve convection and/or radiation on its surfaces exposed to a fluid or other surfaces. Heat transfer is by conduction and possibly by radiation in a still fluid (no bulk fluid motion) and by convection and radiation in a flowing fluid. In the absence of radiation, heat transfer through a fluid is either by conduction or convection, depending on the presence of any bulk fluid motion. Convection = Conduction + Fluid motion Heat transfer through a vacuum is by radiation. Most gases between two solid surfaces do not interfere with radiation. Liquids are usually strong absorbers of radiation. McGraw-Hill | 39 1-10 AEROGEL—A REMARKABLE SUPERINSULATING MATERIAL Aerogels—often called “frozen smoke”—are lightweight and have an ethereal blue haze. An aerogel in your hand feels like a piece of air—but it is a solid. What makes them so interesting is their unique nanoporous structure. This structure is formed through the sol-gel process, whereby a sol (a particulate-containing solution) undergoes a polymerization reaction to form a nanoporous wet gel. The key to making an aerogel is to carefully dry the wet gel. Supercritical extraction is commonly used to make aerogels. Aerogels can be made from many different precursor materials. The most common type of aerogel is the silica aerogel. McGraw-Hill | 40 When an aerogel is made by the sol-gel method, it forms a nanoporous structure comprised of clusters of silica spheres on the order of 5–10 nm that connect and form long, chain-like connecting structures with pores that range from 5 to 100 nm in size. Silica aerogels are very porous: 90–99 percent air Have low density: 0.05–0.4 g/cm3 Large surface areas: 500–1400 m2/g Highly translucent and have low thermal conductivity: 0.01–0.3 W/m⋅K McGraw-Hill | 41 Convection through an aerogel is hindered by the small pore size. At low temperatures radiation is not significant. The primary method for heat transfer through an aerogel is by conduction in both the solid and gaseous phases. Solid phase conduction is related to the thermal conductivity of the solid and the amount of that solid. Since aerogels are so porous, there is very little solid material, and what is there follows a tortuous path with many dead ends (formed by the original sol-gel process). For these reasons, the thermal conductivity of an aerogel is very low. Aerogels are commercially available in an impregnated blanket form, as granules, or as monolithic pieces. They are used in a variety of applications, including comet dust collectors, oil spill clean-up material, and chemical sensors. The most common application for aerogels is as insulation where, for example, they are used in daylighting products (insulating windows), highperformance clothing, and pipe insulation. McGraw-Hill | 42 Heat loss through a 6-mm -thick single-pane glass window If we could make the window pane out of a monolithic aerogel under slight vacuum, the heat loss would be: McGraw-Hill | 43 1-11 PREVENTION THROUGH DESIGN The first of the fundamental canons of ethics for engineers is to “hold paramount the safety, health, and welfare of the public” when fulfilling their professional duties. In 2007, the National Institute for Occupational Safety and Health (NIOSH) launched the National Prevention through Design (PtD) initiative, with the mission to prevent or reduce work-related injuries, illnesses, and fatalities by including prevention considerations in all circumstances that impact individuals in the work places. As such, the concept of PtD involves applying the means of reducing risks and preventing hazards in the design of equipment, tools, processes, and work facilities. The concepts of PtD can also be rationally applied to preventing failures and damages of devices, products, and systems. Since such failures and damages are often led to negative impacts on the environment, profitability, and ultimately the society at large. McGraw-Hill | 44 Within the context of heat and mass transfer, the PtD concepts can be presented along with the physical mechanisms involved and practical applications. Issues such as prevention of thermal burn, fire hazard, and thermal failure in systems are topics that can relate the concepts of PtD with the basic science of heat and mass transfer. The process of solving heat and mass transfer problems, along with the application of PtD concepts, involves incorporating prescribed PtD criteria, the prevention of burn injury, fire hazard, or system failure, to the solutions. To successfully arrive at a solution that satisfies prescribed PtD criteria requires the understanding of how the physical mechanisms of heat and mass transfer interrelate with the concepts of PtD. McGraw-Hill | 45 1-12 ENGINEERING CODES AND STANDARDS Engineering codes and standards are ubiquitous. When we consider any given device that we use daily, the path, from the design to the prototype and finally to the production of the final product is guided by standards and regulated by codes. A product that has been manufactured to meet certain standards tells the user about the product’s quality and that it has met certain levels of scrutiny set forth by those standards. In essence, engineering standards communicate to the user that the product is expected to function safely and meets quality objectives. At the industrial level, engineering codes and standards provide efficiency in engineering processes (from design to manufacturing), maintain safety and uniformity of products that allows interchangeability, and improve commerce. Engineering codes and standards are evolutionary—they are continually revised to reflect technical advances, such as new technologies, new designs, new procedures, and new materials. McGraw-Hill | 46 The development of engineering codes and standards is rooted in the engineers’ code of ethics to “hold paramount the safety, health, and welfare of the public” in their professions (Code of Ethics for Engineers, 2007). The founding of the American Society of Mechanical Engineers (ASME) in 1880 provided a forum for engineers, designers, and machine shop managers to discuss and collaborate to solve issues brought on by the industrial age. Within four years, the first ASME standard, “Code for the Conduct of Trials of Steam Boilers,” was issued. This was the first ASME Performance Test Code (PTC). Today, there are close to 50 ASME PTCs, and they cover components, systems, and facilities. Performance test codes are used by manufacturers to ensure the reliability of their products, and users can use the PTCs to protect themselves from products that function poorly. McGraw-Hill | 47 Some of the very first engineering codes and standards were needed because of engineering failures that caused the loss of life and property. In 1905, a boiler exploded in a shoe factory in Brockton, Massachusetts. In the next year, a similar incident happened in another shoe factory in Lynn, Massachusetts. Within a decade, the first edition of the Boiler and Pressure Vessel Code (BPVC) was issued by the ASME in 1914 and published in 1915. Today, the ASME BPVC has been adopted by the United States and Canada, and it is being used in over 100 countries around the world. A recent study done by ASME Vision 2030 Project reveals that almost 50 percent of engineers in their early career are unfamiliar with engineering codes and standards. As companies and manufacturers expand operations globally, there is a greater need to harmonize codes and standards across jurisdictions and disciplines. The need for engineers to know about codes and standards is growing, and having this knowledge allows engineers to innovate and manufacture competitive products. McGraw-Hill | 48 In the subject of heat and mass transfer, there are several engineering codes and standards that are relevant. These codes and standards have been issued and published by professional associations, such as the ASME and the ASHRAE, and standards organizations, such as ASTM International, the ANSI, and the ISO. For instance, the 2015 ASME Boiler & Pressure Vessel Code, Section IV (ASME BPVC.IV-2015) provided the permitted O-ring materials and their temperature limits for water tube attachments in hot water boilers. Another example is the standard specification issued by ASTM International for polyethylene insulation used on electrical cable (ASTM D1351-14, 2014), which is important as overheating can rapidly deteriorate the insulation. Extreme temperatures and thermal cycles can cause materials to deteriorate and thereby affect the functionality of components. The knowledge of heat and mass transfer, along with adherence to the relevant codes and standards, allow engineers to analyze, design, and build components and systems to function within the design conditions. McGraw-Hill | 49 1-13 PROBLEM-SOLVING TECHNIQUE Step 1: Problem Statement Step 2: Schematic Step 3: Assumptions and Approximations Step 4: Physical Laws Step 5: Properties Step 6: Calculations Step 7: Reasoning, Verification, and Discussion McGraw-Hill | 50 McGraw-Hill | 51 McGraw-Hill | 52 1-14 ENGINEERING SOFTWARE PACKAGES All the computing power and the engineering software packages available today are just tools, and tools have meaning only in the hands of masters. Hand calculators did not eliminate the need to teach our children how to add or subtract, and sophisticated medical software packages did not take the place of medical school training. Neither will engineering software packages replace the traditional engineering education. They will simply cause a shift in emphasis in the courses from mathematics to physics. McGraw-Hill | 53 Equation Solvers Despite its simplicity, Excel is commonly used in solving systems of equations in engineering as well as finance. It enables the user to conduct parametric studies, plot the results, and ask “what if ” questions. It can also solve simultaneous equations if properly set up. Engineering Equation Solver (EES) is a program that solves systems of linear or nonlinear algebraic or differential equations numerically. It has a large library of built-in thermodynamic property functions as well as mathematical functions. Unlike some software packages, equation solvers do not solve engineering problems; they only solve the equations supplied by the user. Therefore, the user must understand the problem and formulate it by applying any relevant physical laws and relations. McGraw-Hill | 54 1-15 ACCURACY, PRECISION, AND SIGNIFICANT DIGITS Accuracy error (inaccuracy): The value of one reading minus the true value. In general, accuracy of a set of measurements refers to the closeness of the average reading to the true value. Accuracy is generally associated with repeatable, fixed errors. Precision error: The value of one reading minus the average of readings. In general, precision of a set of measurements refers to the fineness of the resolution and the repeatability of the instrument. Precision is generally associated with unrepeatable, random errors. Significant digits: Digits that are relevant and meaningful. McGraw-Hill | 55 In engineering calculations, the information given is not known to more than a certain number of significant digits, usually three digits. Consequently, the results obtained cannot possibly be accurate to more significant digits. Reporting results in more significant digits implies greater accuracy than exists, and it should be avoided. McGraw-Hill | 56 Summary • Thermodynamics and Heat Transfer ✓ Application areas of heat transfer ✓ Historical background • Engineering Heat Transfer ✓ Modeling in engineering • Heat and Other Forms of Energy ✓ Specific heats of gases, liquids, and solids ✓ Energy transfer • The First Law of Thermodynamics ✓ Energy balance for closed systems (Fixed Mass) ✓ Energy balance for steady-flow systems ✓ Surface energy balance • Heat Transfer Mechanisms McGraw-Hill | 57 • Conduction ✓ Fourier’s law of heat conduction ✓ Thermal Conductivity ✓ Thermal Diffusivity • Convection ✓ Newton’s law of cooling • Radiation ✓ Stefan–Boltzmann law • Simultaneous Heat Transfer Mechanisms • Aerogel – A Remarkable Superinsulating Material • Prevention through Design • Engineering Codes and Standards • Problem Solving Technique • Engineering Software Packages • Accuracy, Precision and Significant Digits McGraw-Hill | 58 Thank You! 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